Physics:Quantum particles/fermion: Difference between revisions

From HandWiki Test
imported>WikiHarold
Created page with "{{Short description|Particle that obeys the Pauli exclusion principle}} ← Back to Matter by scale A '''fermion''' is a particle that follows Fermi–Dirac statistics and is subject to the Pauli exclusion principle. This means that no two identical fermions can occupy the same quantum state. <div style="float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0..."
 
Finish Quantum residual red link cleanup
 
(4 intermediate revisions by 3 users not shown)
Line 1: Line 1:
{{Short description|Particle that obeys the Pauli exclusion principle}}
{{Short description|Particle that obeys the Pauli exclusion principle}}


[[Book:Quantum Collection/Matter (by scale)|← Back to Matter by scale]]
{{Quantum matter backlink|Particles}}


A '''fermion''' is a [[Physics:Quantum particles/particle|particle]] that follows Fermi–Dirac statistics and is subject to the Pauli exclusion principle. This means that no two identical fermions can occupy the same quantum state.
<div style="display:flex; gap:24px; align-items:flex-start; max-width:1200px;">
 
<div style="width:280px;">
__TOC__
</div>
 
<div style="flex:1; line-height:1.45; color:#006b45; column-count:2; column-gap:32px; column-rule:1px solid #b8d8c8;">
'''fermion''' is a Book II topic in the Quantum Collection. A '''fermion''' is a [[Physics:Quantum particles/particle|particle]] that follows Fermi–Dirac statistics and is subject to the Pauli exclusion principle. This means that no two identical fermions can occupy the same quantum state. Fermions have antisymmetric many-particle wavefunctions, so exchanging two identical fermions changes the sign of the total state. This exchange rule leads to the Pauli exclusion principle and the filling of distinct one-particle states. Fermions include electrons, quarks, neutrinos, protons, neutrons, and many composite systems with half-integer total spin.
</div>
 
<div style="width:300px;">
[[File:Quantum_particles_fermion_concept_map.svg|thumb|280px|fermion in the Quantum Collection.]]
</div>


<div style="float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0 0 1em 1em; width:320px;">
[[File:Fermion_distribution.png|300px]]
<div style="font-size:90%;">Fermions fill available quantum states one by one due to the exclusion principle.</div>
</div>
</div>



Latest revision as of 23:54, 23 May 2026


fermion is a Book II topic in the Quantum Collection. A fermion is a particle that follows Fermi–Dirac statistics and is subject to the Pauli exclusion principle. This means that no two identical fermions can occupy the same quantum state. Fermions have antisymmetric many-particle wavefunctions, so exchanging two identical fermions changes the sign of the total state. This exchange rule leads to the Pauli exclusion principle and the filling of distinct one-particle states. Fermions include electrons, quarks, neutrinos, protons, neutrons, and many composite systems with half-integer total spin.

Error creating thumbnail: File missing
fermion in the Quantum Collection.

Description

Fermions include particles such as quarks and leptons, which make up matter. Their behavior determines the structure of atoms and the stability of matter.

Fermions differ from bosons, which can share quantum states and are not restricted by the exclusion principle.

Properties

  • obey the Pauli exclusion principle
  • cannot share identical quantum states
  • include matter particles

See also

Table of contents (217 articles)

Index

Full contents

References


Author: Harold Foppele


Source attribution: Physics:Quantum particles/fermion